Jessica Taylor. CS undergrad and Master’s at Stanford; former research fellow at MIRI.
I work on decision theory, social epistemology, strategy, naturalized agency, mathematical foundations, decentralized networking systems and applications, theory of mind, and functional programming languages.
Blog: unstableontology.com
Twitter: https://twitter.com/jessi_cata
Yes this is a good approximation.
It’s complicated by i appearing in the Schrodinger equation. Which is essentially a convention. The thing close to ‘replace i with -i in states’ that would produce a real symmetry is CPT.
One thing that quotients out some of this info is the density matrix |ψ⟩⟨ψ|, corresponding to ¯¯¯v⊗v in the post. If H is a Hilbert space, operators H→H have a real structure given by the Hermitian adjoint; and density matrices by definition satisfy conditions including being self-adjoint (i.e. Hermitian, i.e. ρ†=ρ). This means density matrices ‘are real’ in the relevant sense, analogous to real numbers. (Operators representing POVM observables are also self-adjoint/Hermitian.) On the other hand, the derivative of unitary time evolution U’(0) is ‘entirely imaginary’, which is related to the ‘i’ in the Schrodinger equation being conventional.